<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Ogur, S.</author>
             <author>Barnyakov, A.M.</author>
             <author>Furukawa, K.</author>
             <author>Iida, N.</author>
             <author>Levichev, A.E.</author>
             <author>Miyahara, F.</author>
             <author>Nikiforov, D.A.</author>
             <author>Oide, K.</author>
             <author>Papaphilippou, Y.</author>
             <author>Zimmermann, F.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Preliminary Design of FCC-ee Pre-Injector Complex
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-182-3</isbn>
		 <electronic-resource-num>10.18429/JACoW-IPAC2017-TUPAB014</electronic-resource-num>
		 <language>English</language>
		 <pages>1337-1340</pages>
       <pages>TUPAB014</pages>
       <keywords>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2017</year>
          <pub-dates>
             <date>2017-05</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-IPAC2017-TUPAB014</url>
              <url>http://jacow.org/ipac2017/papers/tupab014.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The design of a 100 km circular e⁺e⁻ collider with extremely high luminosity is an important component of the global Future Circular Collider (FCC) study hosted by CERN. FCC-ee is being designed to serve as Z, W, H and top factory, covering beam energies from 45.6 to 175 GeV. For the injectors, the Z-operation is the most challenging mode, due to the high total charge and low equilibrium emittance in the collider at this energy. Thus, fulfilling the Z-mode will also meet the demands for all other modes of FCC-ee. This goal can be achieved by using a 6 GeV NC linac with an S-band RF frequency of 2.856 GHz and a repetition rate of 100 Hz. This linac will accelerate two bunches per RF pulse, each with a charge of 6.5 nC. Positrons will be generated by sending 4.46 GeV e⁻ onto a hybrid target so that the e⁺ created can still be accelerated to 1.54 GeV in the remaining part of the same linac. The emittance of the e⁺ beam will then shrink to the nm level in a 1.54 GeV damping ring. After damping, the e⁺ will be reinjected into the linac and accelerated to 6 GeV. The e⁻ and e⁺ will then be accelerated alternately to 45.6 GeV in the booster, before they are injected into the collider.
       </abstract>
    </record>
  </records>
</xml>
